S. Kumar, R. Tripathi, S. Patra, A. Mhatre, A. Kumar, K. Ramachandran, T. N. Nag, S. Santra
{"title":"Fission product mass distribution studies in 35Cl + 176Yb and 35Cl + 165Ho reactions","authors":"S. Kumar, R. Tripathi, S. Patra, A. Mhatre, A. Kumar, K. Ramachandran, T. N. Nag, S. Santra","doi":"10.1140/epja/s10050-025-01655-w","DOIUrl":null,"url":null,"abstract":"<div><p>Many studies on the fission fragment mass distribution in the sub-lead and pre-actinide region have proposed the presence of asymmetric components in this mass region, primarily due to proton shells corresponding to Z ≈ 36, 38. Present studies have been carried out to investigate the mass distributions in the <sup>35</sup>Cl + <sup>176</sup>Yb → <sup>211</sup>Fr and <sup>35</sup>Cl + <sup>165</sup>Ho → <sup>200</sup>Po reactions in the mass region around ~ 200, a transition between the sub-lead and actinide region. Mass distribution studies have been carried out near the entrance channel Coulomb barrier using the recoil catcher technique, followed by off-line γ-ray spectrometry of the fission products. The broad Gaussian nature of the mass distribution in the <sup>35</sup>Cl + <sup>176</sup>Yb reaction indicates a dominant symmetric fission contribution. The mass distributions for the <sup>35</sup>Cl + <sup>176</sup>Yb and <sup>35</sup>Cl + <sup>165</sup>Ho reactions were found to be in gross agreement with GEF (Schmidt et al<i>.</i> in Nucl Data Sheets 131:107, 2016; Schmidt and Jurado in Rep Prog Phys 81:106301, 2018). The GEF model predicts a dominant symmetric fission contribution along with the contribution from the asymmetric fission mode corresponding to <i>Z</i> ≈ 38. The most probable charge, Z<sub>P</sub> was varied within a range of ± 1.5 units with respect to that obtained using the unchanged charge density hypothesis to obtain the best agreement with GEF. However, a few experimental mass yields in the mass regions corresponding to Z ≈ 50–52 and <i>Z</i> ≈ 54–56 were observed to be still higher (more than ~ 50%) compared to the GEF predictions. A similar enhancement observed in the corresponding fission product yields indicates possible contributions from the conventional asymmetric fission modes, in addition to the shell corresponding to Z ≈ 38.</p></div>","PeriodicalId":786,"journal":{"name":"The European Physical Journal A","volume":"61 8","pages":""},"PeriodicalIF":2.8000,"publicationDate":"2025-08-14","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://link.springer.com/content/pdf/10.1140/epja/s10050-025-01655-w.pdf","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"The European Physical Journal A","FirstCategoryId":"4","ListUrlMain":"https://link.springer.com/article/10.1140/epja/s10050-025-01655-w","RegionNum":3,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q2","JCRName":"PHYSICS, NUCLEAR","Score":null,"Total":0}
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Abstract
Many studies on the fission fragment mass distribution in the sub-lead and pre-actinide region have proposed the presence of asymmetric components in this mass region, primarily due to proton shells corresponding to Z ≈ 36, 38. Present studies have been carried out to investigate the mass distributions in the 35Cl + 176Yb → 211Fr and 35Cl + 165Ho → 200Po reactions in the mass region around ~ 200, a transition between the sub-lead and actinide region. Mass distribution studies have been carried out near the entrance channel Coulomb barrier using the recoil catcher technique, followed by off-line γ-ray spectrometry of the fission products. The broad Gaussian nature of the mass distribution in the 35Cl + 176Yb reaction indicates a dominant symmetric fission contribution. The mass distributions for the 35Cl + 176Yb and 35Cl + 165Ho reactions were found to be in gross agreement with GEF (Schmidt et al. in Nucl Data Sheets 131:107, 2016; Schmidt and Jurado in Rep Prog Phys 81:106301, 2018). The GEF model predicts a dominant symmetric fission contribution along with the contribution from the asymmetric fission mode corresponding to Z ≈ 38. The most probable charge, ZP was varied within a range of ± 1.5 units with respect to that obtained using the unchanged charge density hypothesis to obtain the best agreement with GEF. However, a few experimental mass yields in the mass regions corresponding to Z ≈ 50–52 and Z ≈ 54–56 were observed to be still higher (more than ~ 50%) compared to the GEF predictions. A similar enhancement observed in the corresponding fission product yields indicates possible contributions from the conventional asymmetric fission modes, in addition to the shell corresponding to Z ≈ 38.
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